Слайд 3For ТЕ-waves propagating along Oz axis this is a boundary-value problem for
the equation
Слайд 5First example. 7 layers. The number of ТЕ-modes: K=6.
Слайд 6Traditional dispersion equations –equations for the eigenvalues of the propagation constant
Type
1 – equation, is obtained by equating to zero of the determinant of homogenius linear system due to boundary conditions.
Type 2 ― equation, obtained by the known method of characteristic matrices
This equations have too many terms if the number of layers is more then 4.
Investigation of waveguides with many layers is now actual.
Слайд 7The properties of the dispersion equations
Th.1. Type 1 equation has roots, coinsiding
with the refraction indexes of the inner layers of the waveguide. This roots may not be the eigenvalues of propagation constant.
Th.2. The set of roots of type 2 equation is exactly the set of the eigenvalues of propagation constant.
We propose a new one form of the dispersion equation. This equation in some known cases have no parasitic roots, and moreover it may be treated geometrically.
Слайд 9Homogenius variables,vectors
Слайд 11Theorem 3. Vectors
rotate counter-clockwise when
is decreasing.
Theorem 4. If
then the directions
of this vectors are converging to the direction of Ox axis.
Слайд 12The multilayer equation in vector form
Слайд 13The formulae for the number of TE-modes.
Слайд 15The second example, K=7.
The difference from the first example is only